Lecture 6 Flashcards

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1
Q

4 types of defects, what do defects influence ?

A

point defects
line defects
2D defects
3D defects (bulk).

Defects have a big impact on the properties of the material

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2
Q

4 types of 0D defects, what do they lead to ? consequence ?

A

1) vacancy : missing atom
2) interstitial : not on lattice point
3) large substitution : foreign material
4) small substitution : foreign material

Lattice planes are deformed -> stiffness of material increases

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3
Q

vacancies : what kind of defect, formula at thermal equilibrium, entropy ?

A

thermal defects : number depends on T (higher T = more vacancies).
c_v = exp(-deltaU / R*T).

more vacancies = higher entropy

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4
Q

what does the concentration of vacancies influence ?

A
  • Thermally activated processes such as diffusion
  • segregation
  • plastic deformation
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5
Q

0D defects in ionic crystals : stoichiometric lattices and non-stoichiometric lattices

A

1) stoichiometric (all of same concentration)
- schottky : vacancies on lattice sites
- anti-schottky : vacancies on interstitials
- frenkel : metal vacancies and interstitials
- anti-frenkel : non-metal vacancies and interstitals
- anti-structural disorder : metal on non-metal sires and non-metal on metal sites

2) non-stoichiometric : electrons are redistributed resulting in conductivity -> changes diffusion, deformation, optical properties, …

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6
Q

dislocations : what can generate them, two types, what characterizes them ?

A
  • crystal formation, stress / T gradients, stresses at higher dimensional effects
  • edge and screw
  • burgers vector b : magnitude and direction of lattice distorsion resulting from a dislocation
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7
Q

edge dislocation : what is it, burgers vector

A

Additional half lattice plane.
Vector is perpendicular to dislocation line.

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8
Q

screw disloc : vector ?

A

vector is parallel to dislocation line (step height)

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9
Q

vector when combined disloc ?

A

the vector is neither parallel nor perpendicular to disloc line -> bent

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10
Q

how can a disloc move ? in what direction ? exception ?

A

Under application of force / stress. Gliding only happens in planes, determined by direction of burgers vector.

Only exception is screw disloc : can change the glide plane (cross-gliding)

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11
Q

climbing of dislocations

A

Dislocations move by absorbing or emitting vacancies. When a dislocation absorbs vacancies, it moves upwards, away from the obstacle, and then re-emits vacancies to continue its motion.

strongly dependent on T

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12
Q

dislocation jogs

A

happens when two dislocations interact
(jogs of two screw dislocs are an edge disloc -> hindrance of future movement)

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13
Q

stress and strain in dislocation networks, how can disloc vanish ?

A

Compressive and tensile stresses -> defect clustering.
Edge disloc can vanish if they are opposite type

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14
Q

energy to build a screw disloc ? why do they not exist in thermodynamic equilibrium ?

A

E = Gb^2/4pi * ln(r1/r0)

G = shear modulus (big value)
r0 = radius of disloc nucleus (3 A)
r1 = half mean distance of disloc in solid state (1 micron)

They don’t exist because they are non energetically favorable (in equilibrium, the crystal wants to be at minimal energy state)

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15
Q

burgers vectors in simple lattices

A

fcc : b = a/2<110>
bcc: b = a/2<111> or a<100>
hcp: b = a<11-20> or b = c<0001>

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16
Q

2D lattice defects : what, how can they be formed

A

Stacking faults : created during crystal formation or formed out of dislocations

17
Q

what is a partial disloc ?

A

A partial dislocation has a Burgers vector that is shorter than a unit lattice translation vector for the crystal structure.

18
Q

3D defects, angle ?

A

Grain boundaries with slightly misoriented grains (mosaic).

alpha = a/d when a = interatomic distance, d = distance between edge dislocs

19
Q

order of increased defect densities

A

single crystal < polycrystalline < nanocrystalline < amorphous